The mass spectra of radial and orbital states of doubly heavy baryons are predicted using Hypercentral Constituent Qurk Model (hCQM),by employing screened potential as a confining potential with color-Coulomb potential and compared with references with different theoretical approaches [1]}, [2]}, [3]}, [4]}, [5]}, [6]}, [7]}. As depicted from the tables with comparison, the present results are suppressed especially at higher radial and orbital when compared to linear confining potential appearing in previous work [1]}. In case of [4]} studying using spin-multiplet in HQET, the radial state for spin \(\frac{1}{2}\)  and \(\frac{3}{2}\)  is vary within 100 MeV. For \(\Xi _{bc}\) , only Eakins et al. [3]}, provided few orbital state including \(\frac{5}{2}\) , \(\frac{7}{2}\)  through systematics and symmetries approach which are higher than our results. Our results are underpredicted compared to another non-relativistic approach discussed in ref [2]} as screening effect appears for higher spin configuration. It is noteworthy that our results are on higher side when compared with relativistic approach [6]} and Faddevv approach [5]} available for S and P spin states. For F-state, the mass difference is quite large when compared with Regge phenomenology approach [14]}.
